Radial Friction Bearing with a Fusible Coating in the Turbulent Friction Mode

2019 ◽  
Vol 48 (5) ◽  
pp. 421-430 ◽  
Author(s):  
M. A. Mukutadze ◽  
D. U. Khasyanova
1983 ◽  
Vol 133 ◽  
pp. 207-216 ◽  
Author(s):  
John W. Miles

The evolution of a weakly nonlinear, weakly dispersive gravity wave in water of depth d over a bottom of gradual slope δ and Chezy friction coefficient Cf is studied. It is found that an initially sinusoidal wave evolves into a periodic sequence of solitary waves with relative amplitude a/d = α1 = 15δ/4Cf if α1 < αb, where αb is the relative amplitude above which breaking occurs. This prediction is supported by observations (Wells 1978) of the evolution of swell over mudflats.


Nature ◽  
1966 ◽  
Vol 212 (5065) ◽  
pp. 874-877 ◽  
Author(s):  
G. E. GADD
Keyword(s):  

SPE Journal ◽  
2000 ◽  
Vol 5 (02) ◽  
pp. 182-189 ◽  
Author(s):  
Jun Xu ◽  
S.A. Shirazi ◽  
D.R. Doty ◽  
M.G. Prado ◽  
R.N. Blais
Keyword(s):  

2021 ◽  
Vol 410 ◽  
pp. 439-443
Author(s):  
Vladislav R. Baraz ◽  
Svetlana Kh. Estemirova ◽  
Elena A. Ishina

The peculiarities of the microstructure and properties of BrBNT1.7 beryllium bronze tape samples were studied: the samples were subjected to dispersion hardening as a result of quenching in a supersaturated solid solution and aging. Friction deformation in a dry friction mode provides additional effective hardening while maintaining increased plasticity (bending-and-unbending test).


2012 ◽  
Vol 69 (11) ◽  
pp. 3097-3115 ◽  
Author(s):  
B. J. H. Van de Wiel ◽  
A. F. Moene ◽  
H. J. J. Jonker

Abstract The mechanism behind the collapse of turbulence in the evening as a precursor to the onset of the very stable boundary layer is investigated. To this end a cooled, pressure-driven flow is investigated by means of a local similarity model. Simulations reveal a temporary collapse of turbulence whenever the surface heat extraction, expressed in its nondimensional form h/L, exceeds a critical value. As any temporary reduction of turbulent friction is followed by flow acceleration, the long-term state is unconditionally turbulent. In contrast, the temporary cessation of turbulence, which may actually last for several hours in the nocturnal boundary layer, can be understood from the fact that the time scale for boundary layer diffusion is much smaller than the time scale for flow acceleration. This limits the available momentum that can be used for downward heat transport. In case the surface heat extraction exceeds the so-called maximum sustainable heat flux (MSHF), the near-surface inversion rapidly increases. Finally, turbulent activity is largely suppressed by the intense density stratification that supports the emergence of a different, calmer boundary layer regime.


1973 ◽  
Vol 16 (91) ◽  
pp. 93-99 ◽  
Author(s):  
Tomosada JOTAKI ◽  
Yuji TOMITA

1979 ◽  
Vol 101 (3) ◽  
pp. 469-474 ◽  
Author(s):  
A. T. Wassel ◽  
A. F. Mills

A numerical calculation method for turbulent flow in rough pipes is developed. A mixing length model is used in the turbulent core while a roughness element drag coefficient and a sub-layer Stanton number are used to characterize transport to the wall. Sample wall relations are developed for sandgrain roughness and transverse repeated rib roughness, and it is shown that large roughness heights require accounting for terms of order of roughness height divided by pipe radius. For gas flows with cooling, the effects of variable properties are investigated for smooth walls and both roughness patterns. For smooth walls, comparison with experiment is satisfactory; for rough walls experimental data is not available. Simple power law formulae representing variable property effects for fully rough flows are presented.


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